2025ApJ...991..151B


Query : 2025ApJ...991..151B

2025ApJ...991..151B - Astrophys. J., 991, 151 (2025/October-1)

Blue Supergiants in the Pinwheel Galaxy M101: Comparison with H II Region Chemical Abundances, Spectroscopic Distance, and an Independent Determination of the Hubble Constant.

BRESOLIN F., KUDRITZKI R.-P., URBANEJA M.A., SEXTL E. and RIESS A.G.

Abstract (from CDS):

We present a quantitative spectroscopic study of 13 blue supergiant stars in the Pinwheel Galaxy M101, based on data obtained with the Low Resolution Imaging Spectrometer available at the Keck I telescope. The average stellar metallicity decreases from ∼1.9 Z⊙ near the center of the galaxy to ∼0.3 Z⊙ at the optical outskirts. The galactocentric radial metallicity gradient is statistically consistent with previous studies of the gas-phase oxygen abundance from H II regions using the direct method. The H II region-based Cepheid metallicities used by A. G. Riess et al. in their determination of the Hubble constant H0 are in substantial agreement with our measurements. The direct method gas-phase metallicities of the 18 star-forming galaxies we have analyzed so far, when adjusted upward for a mean ∼0.15 dex oxygen dust depletion factor, are in good agreement with those we infer from the supergiants, over a factor of 50 in metallicity. From the same data, we derive an expression for the metal-dependent depletion of oxygen in photoionized nebulae. Utilizing the flux-weighted gravity-luminosity relationship (FGLR) of blue supergiants, we measure a distance to M101, D = 6.5 ± 0.2 Mpc (μ = 29.06 ± 0.08), which is within 1σ from determinations based on the tip of the red giant branch and Cepheids. With M101 as a nearby Type Ia supernova host and using the observed standardized B-band magnitude of the supernova, our FGLR distance yields an independent value of H0 = 72.5 ± 4.6 km s–1 Mpc–1.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Stellar abundances - Galaxy abundances - Galaxy stellar content - Stellar distance - Hubble constant - Supergiant stars - Spectroscopy - Chemical abundances

Simbad objects: 62

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Number of rows : 62
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 MCG-03-01-015 G 00 01 57.9 -15 27 50   11.50 11.10 10.93   ~ 782 2
2 NGC 55 rG 00 14 53.602 -39 11 47.86 8.54 8.58 7.87 7.84   ~ 828 2
3 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
4 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
5 NGC 300 GiG 00 54 53.4465638304 -37 41 03.168402396 8.83 8.69 8.13 7.46   ~ 1614 2
6 IC 1613 GiC 01 04 48.4071 +02 07 10.185   10.42 10.01 9.77   ~ 1316 2
7 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
8 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
9 NGC 1365 Sy1 03 33 36.458 -36 08 26.37 10.48 10.08 9.63 8.79 9.7 ~ 1987 2
10 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
11 M 42 HII 05 35 16.8 -05 23 15           ~ 4411 0
12 NGC 2403 AGN 07 36 51.3381434280 +65 36 09.650825640 9.31 8.84 8.38 8.19   ~ 1887 1
13 M 81 Sy2 09 55 33.1726556496 +69 03 55.062505368   7.89 6.94     ~ 4725 3
14 Z 153-10 G 09 59 26.46 +30 44 47.0 14.08 13.54 13.26 13.33   ~ 652 0
15 NGC 3109 AG? 10 03 06.877 -26 09 34.46 11.10 10.42 10.04 9.91   ~ 825 2
16 NGC 3621 Sy2 11 18 16.300 -32 48 45.36 10.10 9.44 9.56 8.07 10.1 ~ 661 3
17 M 106 Sy2 12 18 57.620 +47 18 13.39   9.14 8.41 8.11   ~ 2512 4
18 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2778 2
19 [GH2013b] J140219.69+541913.58 s*b 14 02 19.69 +54 19 13.6   21.194 21.001   20.872 A2I 1 0
20 [GH2013b] J140221.39+542151.73 s*b 14 02 21.39 +54 21 51.7   21.205 20.985   20.704 A5I 1 0
21 [GH2013b] J140225.55+541917.18 s*b 14 02 25.55 +54 19 17.2   20.997 20.848   20.71 A1I 1 0
22 [GH2013b] J140226.24+541944.04 s*b 14 02 26.24 +54 19 44.0   20.773 20.687   20.753 B5I 1 0
23 [GH2013b] J140228.23+542004.02 s*b 14 02 28.23 +54 20 04.0   21.576 21.441   21.304 ~ 1 0
24 [GH2013b] J140233.31+542153.57 s*b 14 02 33.31 +54 21 53.6   21.428 21.349   21.337 B5/B6I 1 0
25 [GH2013b] J140237.36+542151.66 s*b 14 02 37.36 +54 21 51.7   21.357 21.342   21.569 ~ 1 0
26 [GH2013b] J140242.59+542036.35 s*b 14 02 42.59 +54 20 36.4   20.782 20.627   20.469 A2I 1 0
27 [GH2013b] J140244.33+542010.64 s*b 14 02 44.33 +54 20 10.6   21.295 21.093   20.845 A2I 2 0
28 [GH2013b] J140248.46+541935.80 s*b 14 02 48.4790667000 +54 19 35.725848924   20.29 20.105   19.883 A2,HIII 2 0
29 [GH2013b] J140251.72+542029.15 s*b 14 02 51.72 +54 20 29.1   21.362 21.165   20.992 A2I 1 0
30 [GH2013b] J140253.64+542319.25 s*b 14 02 53.64 +54 23 19.2   21.642 21.417   21.153 ~ 1 0
31 [GH2013b] J140254.07+541942.89 s*b 14 02 54.07 +54 19 42.9   20.765 20.728   20.668 B7/B8I 1 0
32 [GH2013b] J140256.68+542018.20 s*b 14 02 56.68 +54 20 18.2   21.247 21.161   21.039 ~ 1 0
33 [GH2013b] J140300.02+542102.88 s*b 14 03 00.02 +54 21 02.9   21.438 21.280   21.024 ~ 1 0
34 [GH2013b] J140302.24+542032.28 s*b 14 03 02.24 +54 20 32.3   21.269 21.168   21.025 A2I 1 0
35 [GH2013b] J140303.02+542110.12 s*b 14 03 03.02 +54 21 10.1   21.549 21.421   21.292 A2I 1 0
36 [GH2013b] J140303.83+542330.88 s*b 14 03 03.83 +54 23 30.9   20.823 20.577   20.346 A7I 1 0
37 [GH2013b] J140305.68+541845.68 s*b 14 03 05.68 +54 18 45.7   21.42 21.367   21.284 B8I 1 0
38 SN 2011fe SN* 14 03 05.711 +54 16 25.22   10.12 10.06     SNIa-norm 747 1
39 [GH2013b] J140306.55+542048.19 s*b 14 03 06.55 +54 20 48.2   20.99 20.840   20.632 ~ 1 0
40 [GH2013b] J140306.66+542125.24 s*b 14 03 06.66 +54 21 25.2   21.378 21.107   20.812 ~ 1 0
41 [GH2013b] J140308.01+542031.13 s*b 14 03 08.01 +54 20 31.1   21.318 21.144   20.91 ~ 1 0
42 M 101 GiP 14 03 12.583 +54 20 55.50   8.46 7.86 7.76   ~ 3138 2
43 [GH2013b] J140312.61+542043.66 s*b 14 03 12.6225579984 +54 20 43.647686808   20.537 20.404   20.203 ~ 2 0
44 [GH2013b] J140313.44+541954.37 s*b 14 03 13.44 +54 19 54.4   21.913 21.870   22.303 ~ 1 0
45 [GH2013b] J140313.86+541845.54 s*b 14 03 13.86 +54 18 45.5   21.498 21.343   21.097 ~ 1 0
46 [GH2013b] J140315.26+542039.30 s*b 14 03 15.26 +54 20 39.3   20.98 20.705   20.426 A7I 1 0
47 [GH2013b] J140316.61+541654.84 s*b 14 03 16.61 +54 16 54.8   21.25 21.046   20.831 ~ 1 0
48 [GH2013b] J140320.66+542208.04 s*b 14 03 20.66 +54 22 08.0   21.399 21.215   21 B8/B9I 1 0
49 [GH2013b] J140320.68+541649.58 s*b 14 03 20.68 +54 16 49.6   21.532 21.482   21.404 ~ 1 0
50 [GH2013b] J140321.66+542157.71 s*b 14 03 21.66 +54 21 57.7   21.157 21.066   20.927 A3I 1 0
51 [GH2013b] J140324.77+541726.74 s*b 14 03 24.77 +54 17 26.7   21.054 20.899   20.688 A2I 1 0
52 [GH2013b] J140325.68+541644.87 s*b 14 03 25.68 +54 16 44.9   20.874 20.656   20.386 A3I 1 0
53 [GH2013b] J140328.50+542128.37 s*b 14 03 28.50 +54 21 28.4   21.208 20.941   20.703 ~ 1 0
54 [GH2013b] J140328.91+542026.88 s*b 14 03 28.91 +54 20 26.9   21.587 21.490   21.339 ~ 1 0
55 [GH2013b] J140328.91+542350.24 s*b 14 03 28.91 +54 23 50.2   21.292 21.237   21.176 ~ 1 0
56 [GH2013b] J140329.44+542343.37 s*b 14 03 29.44 +54 23 43.4   21.183 21.054   20.927 ~ 1 0
57 [GH2013b] J140332.31+541751.83 s*b 14 03 32.31 +54 17 51.8   21.5 21.383   21.179 ~ 1 0
58 [GH2013b] J140334.78+541810.22 s*b 14 03 34.78 +54 18 10.2   21.523 21.473   21.449 B2I 1 0
59 [GH2013b] J140336.78+542155.37 s*b 14 03 36.78 +54 21 55.4   20.492 20.434   20.422 B4I 1 0
60 [GH2013b] J140338.08+541845.61 s*b 14 03 38.08 +54 18 45.6   21.172 20.957   20.7 A0/A2I 1 0
61 [GH2013b] J140339.78+541829.74 s*b 14 03 39.78 +54 18 29.7   21.405 21.363   21.396 ~ 1 0
62 [GH2013b] J140342.56+541902.60 s*b 14 03 42.56 +54 19 02.6   21.119 21.030   20.959 ~ 1 0

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